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Reversible diffusion-controlled reactions

A partially absorbing boundary is equivalent to a finite strength, delta-function sink located at the boundary [75] the sink does not need to coincide with the boundary. Theory [70, 71] was successfully applied to reversible reactions of isolated (geminate) pairs but its generalizations to pseudo-first [Pg.288]

Smoluchowski approximation for noninteracting B s and independent AB pairs turned out to be non-trivial problem (see also [76]). Even when the Smoluchowski theory for irreversible pseudo-first-order reactions is exact, no rigorous theory that is valid for an arbitrary set of kinetic ptirameters was developed in [70] the additional assumption was made that every time a bound AB pair dissociates forming an unbound pair at contact, this pair behaves as if it was surrounded by an equilibrium distribution of B s independent of the history of previous associations and dissociations (see also [77]). [Pg.289]

Approximate treatment of the many-particle effects in reversible bimolecular reactions has been undertaken in several papers (see for a review [78]) we would like also to note here pioneering studies of Ovchinnikov s group [79-82] and Kang and Redner s paper [83]. The former approach was discussed above in Section 2.1.2.3 where the kinetics of the approach to equilibrium for the simple reaction A B -f B (dissociation and association of molecules A) was shown to approach the equilibrium as Note also that in the paper [84] a new elegant quantum-field formalism has been developed for the first time and applied to the diffusion-controlled reactions in the fluctuation regime its results agree completely with the phenomenological estimate (2.1.61). [Pg.289]

It should be stressed that despite the same critical exponent, a = 3/2, was obtained in studies of reversible reaction A B -I- B discussed above [Pg.289]

It should be stressed that the reversible chemical reactions give us better chance to observe many-particle effects since there is no need here to monitor vanishing particle concentrations over many orders of magnitude. Indeed, the fluctuation-controlled law of the approach to the reaction equilibrium similar to (2.1.61) was observed recently experimentally [85] for the pseudo-first-order reaction A-l-B AB of laser-excited ROH dye molecules which dissociate in the excited state to create a geminate proton-excited anion pair. The solvated proton is attracted to the anion and recombines with it reversibly. After several dissociation-association cycles it finally diffuses to long distances and further recombination becomes unobservable. [Pg.290]


As a first step, it is important to define which reactions are susceptible to be catalyzed. In principle, the reaction rates of any process can be increased. In a heterogeneous process, such as electrode reactions, the diffusion of the active species to the electrode may be the rate-determining step of the whole process. In that case, any improvement in the rate of the electron-transfer step would not produce any change in the overall rate of the process, since the mass-transfer process is still the limiting step. The electrode reaction will behave then as a reversible diffusion-controlled reaction. Whenever the reaction in the actual experimental conditions is not diffusion controlled, it may be interesting to find a better electrocatalyst for it. The criteria for defining a reaction as diffusion controlled depends on the technique employed for the study. According to the technique, several... [Pg.975]

Cyclic voltammetry provides both quahtative and quantitative information on electrode processes. A reversible, diffusion-controlled reaction such as presented by Eq. (2.9) exhibits an approximately symmetrical pair of current peaks, as shown in Fig. 2.20. The voltage separation AE of these peaks is... [Pg.56]

Pulse radiolysis studies showed that the rate of the reaction of MV with a-Fc203, in which an electron is transferred to the colloidal particles, is slower than predicted for a diffusion controlled reaction. For pH > 8, the reaction is incomplete as the reverse reaction Fe203 - - - Fe203 - - MV takes place more efficiently... [Pg.159]

The first cathodic wave was studied by cycling the potential across it at various scan rates and the peak potentials were found to increase as indicative of a reversible, diffusion-controlled system, with ° = — 1.43 V vs. SCE. However, at sweep rates 20mV/s the peak anodic current is much smaller than expected which was interpreted by the authors as indicating that the reduced species undergoes a subsequent chemical reaction, i.e. an EC process. [Pg.314]

In addition to this, and in contrast with the homogeneous case discussed in Section 5.2.2, the diffusion of P and Q is therefore not perturbed by any homogeneous reaction. If, furthermore, the P/Q electron transfer at the electrode is fast and thus obeys Nernst s law, the diffusive contribution to the current in equations (5.11) and (5.12) is simply equal to the reversible diffusion-controlled Nernstian response, idif, discussed in Section 1.2. The mutual independence of the diffusive and catalytic contributions to the current, expressed as... [Pg.316]

The above expression for has been derived from free volume considerations (17) as well as from the forward and reverse rates of diffusion-controlled reactions (18) the expression for w is valid when the radii of all the ions are equal. The relation between the above formulation and eq 1 may be seen from the following considerations. If most of the contribution to the observed rate comes from electron transfer over a small range of r values then... [Pg.111]

The cathodic pinacolisation of 2- and 4-acetylpyridine, which had been investigated by one of the present authors (231-233), offered the chance for a complete kinetic analysis as the respective current voltage curves are of reversible character. They allow for evaluation of the kinetics of consecutive reactions, and one can show that at low pH reaction, Eq. (45c) is only possible if strong surfactants are absent. Such surfactants, by occupying the electrode surface, displace ketyl radicals, RiR2(OH)C , from the electrode surface because the latter are relatively weakly adsorbed and cannot compete with strong surfactants in adsorption. Ketyl radicals dissolved in aqueous or organic solvents of low pH are protonated in a fast almost diffusion-controlled reaction. After protonation they are further immediately reduced to form the monomeric carbinol instead of the hydrodimer—the pinacol ... [Pg.165]

In our opinion, this book demonstrates clearly that the formalism of many-point particle densities based on the Kirkwood superposition approximation for decoupling the three-particle correlation functions is able to treat adequately all possible cases and reaction regimes studied in the book (including immobile/mobile reactants, correlated/random initial particle distributions, concentration decay/accumulation under permanent source, etc.). Results of most of analytical theories are checked by extensive computer simulations. (It should be reminded that many-particle effects under study were observed for the first time namely in computer simulations [22, 23].) Only few experimental evidences exist now for many-particle effects in bimolecular reactions, the two reliable examples are accumulation kinetics of immobile radiation defects at low temperatures in ionic solids (see [24] for experiments and [25] for their theoretical interpretation) and pseudo-first order reversible diffusion-controlled recombination of protons with excited dye molecules [26]. This is one of main reasons why we did not consider in detail some of very refined theories for the kinetics asymptotics as well as peculiarities of reactions on fractal structures ([27-29] and references therein). [Pg.593]

Figure 9. Recovered forward (a) and reverse ( ) rates for the excimer system described in Figure 1 compared to that expected for a diffusion-controlled reaction (o). Figure 9. Recovered forward (a) and reverse ( ) rates for the excimer system described in Figure 1 compared to that expected for a diffusion-controlled reaction (o).
Simple olefins do not react with eaq at an appreciable rate, but compounds with an extended 7t-system such as butadiene can also accommodate an additional electron (k = 8 x 109 dm3 mol-1 s 1 Hart et al. 1964). However, as in the case of benzene, the rate is often below diffusion controlled [reaction (23) k = 7.2 x 106 dm3 mol 1 s 1 (Gordon et al. 1977) in THF, the reaction of the solvated electron with benzene is even reversible (Marasas et al. 2003)], and the resulting radical anion is rapidly protonated by water [reaction (24)]. [Pg.83]

In the case of a diffusion-controlled reaction a current-potential curve can be evaluated quantitatively. The diffusion equation has to be solved again by using time-dependent boundary conditions. The mathematics, however, are very complicated and cannot be shown here. They end up with an integral equation which has to be solved numerically [11]. The peak current, /p, for a diffusion-controlled process (reversible reaction) is found to be... [Pg.163]

The rate of proton dissociation is controlled by three parameters the frequency of ion pair formation, the rate of stabilization of the proton by hydration, and the rate of escape out of the Coulomb cage. Measurements carried out in dilute salt solutions, that is, 10— lOOmM, will not be influenced by the two later steps. The activity of the water is invariable whereas the ionic atmosphere will screen the electrostatic attraction. Under such conditions, the rate of dissociation should be a direct function of the probability that the stretching covalent bond will reach the dissociation distance. As demonstrated in Figure 2, this expected correlation is observed over a wide range of pKs. Under these conditions, a reversible dissociation will comply with the relationship Kdiss = ki/k-i. As the recombination reaction for all acids is a diffusion-controlled reaction, we can approximate = k-t Kdlss — 1010 Kdiss(sec-1). [Pg.10]

The complex [Ru" (HL)(H20)] (1 mM) at pH 2.8 showed a pair of cathodic and anodic peaks at -0.236 and -0.173 V respectively for Ru"V Ru redox couple (Figure 2B.a). The peak current were proportional to square root of scan speeds, ratio of anodic to cathodic currents was close to imity, peak separation (AEp) was 60 mV and Ep/2-Ep 63 mV were the characteristic features for one electron quasi-reversible and diffusion controlled reaction. [Pg.522]

The rate constant for the reverse of Reaction 1 is 1.8 X 107 liter/mole sec. (5). This value is somewhat less than would be expected for a diffusion controlled reaction. If the pre-exponential factor is near the 1010 liter/mole sec. considered normal for an activation-controlled reaction of an ion with a neutral molecule, the Arrhenius energy of activation would be about 3.8 kcal./mole in reasonable agreement with the value of 4.5 kcal./mole based on the AHr entry in Table II. Since the transition state for Reaction 1 almost certainly has negative charge more dispersed than in the neighborhood of an hydroxide ion, the pre-exponential term for the reverse reaction may even be somewhat more positive than the normal 1010 liter/mole sec., and the enthalpy of activation would then be larger also. Even if the correct enthalpy of activation is less than the value quoted in Table II, the difference could hardly be more than 2 kcal./mole. [Pg.74]

Electron and proton transfer reactions between natural products are, with the exception of C-H bond cleavage, very fast. Essentially each single collision between a donor and acceptor leads to a reaction ((diffusion controlled (reaction) and velocity constants are in the order of k = 10 ° mol s. Proton exchange between water molecules is an example of such a reaction. It has no mechanism and obeys the thermodynamic laws of reversible processes. [Pg.29]

A second type of transient SECM experiment is double potential step chronoam-perometry in which the species generated at the tip under diffusion control in the first potential step reacts at or is transferred across a nearby interface. As the rate of the interfacial reaction increases, the fraction collected in the reverse potential step is reduced. At short times, the current during the reverse step varies linearly with and there are two limiting slopes corresponding to the cases of no reaction at the interface to that of diffusion-controlled reaction at the interface. For intermediate cases, the interfacial kinetics may be extracted [88]. [Pg.459]


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See also in sourсe #XX -- [ Pg.288 , Pg.593 ]

See also in sourсe #XX -- [ Pg.288 , Pg.593 ]




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Diffusion control

Diffusion controlled

Diffusion reaction control

Diffusion reactions

Diffusion reverse

Diffusion-controlled reactions

Diffusivity reactions

Reaction reverse

Reaction reversible

Reactions, reversing

Reversibility Reversible reactions

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